Additional lemmas for interval integrals #
This file records general-purpose lemmas about interval integrals ∫ x in a..b, f x ∂μ that do
not belong to any particular application.
Main results #
TauCeti.intervalIntegral.monotoneOn_primitive_of_nonneg: the primitivet ↦ ∫ x in a..t, f xof a function that is nonnegative and interval integrable on[a, b]is nondecreasing on[a, b].TauCeti.intervalIntegral.eq_of_integral_eq_sub: if the increments ofFare the interval integrals of a function vanishing outside[-r, r]with total integral zero, thenFis constant outside[-r, r].TauCeti.intervalIntegral.integral_re_mul_im_sub_im_mul_re_eq: a polarization identity expressing∫ (x v - y u)forf = x + i yandg = u + i vthrough the integrals of‖g‖²,‖f‖²and‖g - i k f‖².TauCeti.intervalIntegral.norm_sub_sub_integral_le: the defecta₂ - a₁ - ∫ gfrom an integral equation changes by at most the changes of the endpoint values plusδ |t₂ - t₁|when the integrand changes by at mostδ.TauCeti.tendsto_intervalIntegral_atTop_atBot: the accumulated integral of a locally integrable function bounded below almost everywhere by a positive constant tends to+∞at+∞and to-∞at-∞.MeasureTheory.IntegrableOn.intervalIntegrable_of_mem_Icc: a function integrable on(a, b)for a measure without mass at points is interval integrable between any two points of[a, b].ContinuousLinearEquiv.intervalIntegral_comp_comm: a continuous linear equivalence commutes with interval integrals, with no integrability assumption.MeasureTheory.LocallyIntegrableOn.intervalIntegrable_comp_max: iffis locally integrable on[c, ∞), then its constant extensionx ↦ f (max x c)is interval integrable on every interval.
The primitive t ↦ ∫ x in a..t, f x ∂μ of a function that is almost everywhere nonnegative and
interval integrable on [a, b] is nondecreasing on [a, b].
If the increments of F are the interval integrals of a function f that vanishes outside
[-r, r] and has total integral zero, then F is constant outside [-r, r].
A polarization identity for complex functions f = x + i y and g = u + i v, square
integrable on uIoc a b: for real k ≠ 0,
∫ₐᵇ (x v - y u) = (∫ₐᵇ ‖g‖² + k² ∫ₐᵇ ‖f‖² - ∫ₐᵇ ‖g - i k f‖²) / (2k).
For a curve f with velocity g, the left side is twice the signed area of f.
The defect a₂ - a₁ - ∫ g from an integral equation over [t₁, t₂] differs from the defect
b₂ - b₁ - ∫ g' by at most ‖a₁ - b₁‖ + ‖a₂ - b₂‖ + δ |t₂ - t₁| when ‖g - g'‖ ≤ δ on the
interval.
A function vanishing on (-∞, a] and on a ball around a has zero integral on a..t for
every t < a + ε, where ε is the radius of that ball.
The primitive of a step velocity corrected by its average defect reaches the prescribed endpoint.
The accumulated integral t ↦ ∫ r in a..t, w r of a locally integrable function bounded below
almost everywhere by a positive constant tends to +∞ at +∞ and to -∞ at -∞.
A function integrable on (a, b) for a measure without mass at points is interval integrable
between any two points s, t ∈ [a, b].
A continuous linear equivalence commutes with interval integrals of arbitrary functions;
compare ContinuousLinearMap.intervalIntegral_comp_comm, which needs integrability.
If f is locally integrable on [c, ∞) for a locally finite measure, then its constant
extension x ↦ f (max x c) to all of ℝ is interval integrable between any two points.